EP2280470B1 - Elément de champ - Google Patents

Elément de champ Download PDF

Info

Publication number
EP2280470B1
EP2280470B1 EP09742670.4A EP09742670A EP2280470B1 EP 2280470 B1 EP2280470 B1 EP 2280470B1 EP 09742670 A EP09742670 A EP 09742670A EP 2280470 B1 EP2280470 B1 EP 2280470B1
Authority
EP
European Patent Office
Prior art keywords
field
insertion holes
magnet insertion
circumferential direction
field magnet
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Not-in-force
Application number
EP09742670.4A
Other languages
German (de)
English (en)
Other versions
EP2280470A1 (fr
EP2280470A4 (fr
Inventor
Keiji Aota
Yoshihito Sanga
Akio Yamagiwa
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Daikin Industries Ltd
Original Assignee
Daikin Industries Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Daikin Industries Ltd filed Critical Daikin Industries Ltd
Publication of EP2280470A1 publication Critical patent/EP2280470A1/fr
Publication of EP2280470A4 publication Critical patent/EP2280470A4/fr
Application granted granted Critical
Publication of EP2280470B1 publication Critical patent/EP2280470B1/fr
Not-in-force legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • H—ELECTRICITY
    • H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02K—DYNAMO-ELECTRIC MACHINES
    • H02K1/00—Details of the magnetic circuit
    • H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/22—Rotating parts of the magnetic circuit
    • H02K1/27—Rotor cores with permanent magnets
    • H02K1/2706—Inner rotors
    • H02K1/272—Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis
    • H02K1/274—Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets
    • H02K1/2753—Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets the rotor consisting of magnets or groups of magnets arranged with alternating polarity
    • H02K1/276—Magnets embedded in the magnetic core, e.g. interior permanent magnets [IPM]
    • H—ELECTRICITY
    • H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02K—DYNAMO-ELECTRIC MACHINES
    • H02K1/00—Details of the magnetic circuit
    • H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/22—Rotating parts of the magnetic circuit
    • H02K1/27—Rotor cores with permanent magnets
    • H02K1/2706—Inner rotors
    • H02K1/272—Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis
    • H02K1/274—Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets
    • H02K1/2753—Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets the rotor consisting of magnets or groups of magnets arranged with alternating polarity
    • H02K1/276—Magnets embedded in the magnetic core, e.g. interior permanent magnets [IPM]
    • H02K1/2766—Magnets embedded in the magnetic core, e.g. interior permanent magnets [IPM] having a flux concentration effect

Definitions

  • the present invention relates to a field element, and more particularly, to an embedded type field element.
  • JP-A-2003-88015 describes an interior permanent magnet rotor capable of reducing cogging torque.
  • the rotor includes a rotor core and four permanent magnets that are built and disposed in the rotor core. These permanent magnets are circularly disposed with a rotation axis being the center.
  • An outer contour of the rotor core has a so-called petal shape in which the radius on both end sides of the permanent magnets is smaller than the radius on the center side of the permanent magnets in a circumferential direction with the rotation axis being the center.
  • a magnetic field distribution of a magnetic flux density distribution is improved, so that the magnetic flux density distribution is made close to a sinusoidal distribution.
  • US 2005/0200223 A1 discloses a permanent magnet rotating electric machine that comprises a stator having stator windings wound round a stator iron core and a permanent magnet rotor having a plurality of inserted permanent magnets in which the polarity is alternately arranged in the peripheral direction in the rotor iron core.
  • the rotor iron core of the permanent magnets is composed of magnetic pole pieces, auxiliary magnetic poles, and a stator yoke, and furthermore has concavities formed on the air gap face of the magnetic pole pieces of the rotor iron core of the permanent magnets, gently tilting from the central part of the magnetic poles to the end thereof.
  • US 2007/0126304 A1 discloses a rotary shaft having an outside diameter larger than the bore diameter of a rotary shaft insert hole of a rotor is inserted into the rotary shaft insert hole.
  • a magnet insert hole is provided in a main magnetic pole of the rotor. Permanent magnets to are inserted into the magnet insert hole such that a gap is formed between the permanent magnets and the magnet insert hole.
  • a semi-tubular rivet insert hole and interlocks elongated in the radial direction of the rotor are disposed radially outward of the magnet insert hole in the rotor.
  • a semi-tubular rivet is inserted into the semi-tubular rivet insert hole such that a gap is formed between the semi-tubular rivet and the semi-tubular rivet insert hole. Passage holes, are provided in the auxiliary magnetic poles.
  • JP 2001 178045 A discloses a magnet housing holes the cross section in the axial direction, of which is trapezoidal in shape, with its projected side facing toward the center are formed in a rotor core. Permanent magnets are embedded in the magnet housing holes. A notched portion, cut from end walls of the magnet housing holes in the direction of the outer circumference of the rotor core is formed in the portion of the rotor core, opposed to the end walls. Or a gap is formed between the end walls and the outer circumferential wall of the rotor core.
  • An object of the present invention is therefore to provide a field element capable of easily measuring an air gap at both ends of the permanent magnets while reducing cogging torque.
  • a field element includes: a plurality of field magnets (20, 21, 22); and a field element core (1) having a perimeter (10) exposed around a predetermined axis (P), and a plurality of field magnet insertion holes (30, 31, 33) disposed circularly around the axis, at least one of the plurality of field magnets is inserted into each of said at least one of said plurality of field magnet insertion holes, wherein: the at least one of the plurality of field magnets inserted into each of the plurality of field magnet insertion holes is disposed with magnetic pole surfaces of a single polarity facing the perimeter; one of the plurality of field magnet insertion holes and another of the plurality of field magnet insertion holes are adjacent to each other in a circumferential direction (D) with the axis being a center, where the magnetic pole surface of the at least one of the plurality of field magnets inserted into the one of the plurality of field magnet insertion holes and the magnetic pole surface of the at least one of the plurality
  • each of the plurality of field magnet insertion holes has, at both ends in the circumferential direction (D), first cavity portions (31) on a side closer to the perimeter (10) than the at least one of the plurality of field magnets (21, 22) inserted thereinto;
  • the field element core (1) further has second cavity portions (32) each disposed along the perimeter on the first position (101) side with respect to the first cavity portion, apart from the first cavity portion in the circumferential direction (D); and a point (11) on the perimeter at which the distance (R) turns from decreasing to increasing between the first position and the second position is positioned on a side closer to the second position in the circumferential direction than an end (321) on the first position side of the second cavity portion in the circumferential direction.
  • a field element includes: a plurality of field magnets (20, 21, 22); and a field element core (1) having a perimeter (10) exposed around a predetermined axis (P), and a plurality of field magnet insertion holes (30, 31, 33) disposed circularly around the axis, at least one of the plurality of field magnets is inserted into each of said at least one of said plurality of field magnet insertion holes, wherein: the at least one of the plurality of field magnets inserted into each of the plurality of field magnet insertion holes is disposed with magnetic pole surfaces of a single polarity facing the perimeter; one of the plurality of field magnet insertion holes and another of the plurality of field magnet insertion holes are adjacent to each other in a circumferential direction (D) with the axis being a center, where the magnetic pole surface of the at least one of the plurality of field magnets inserted into the one of the plurality of field magnet insertion holes and the magnetic pole surface of the at least one
  • the center of the one of the plurality of field magnet insertion holes in the circumferential direction (D) is positioned on the axis (P) side with respect to a straight line connecting both ends in the circumferential direction of the at least one of the plurality of field magnets inserted into the one of the plurality of field magnet insertion holes (30).
  • a holding force of the at least one of the plurality of field magnets (20) is larger on an end portion side of the field magnet insertion hole in the circumferential direction than on the center side of the plurality of field magnet insertion holes (30) into which itself is inserted.
  • an energy product of the at least one of the plurality of field magnets (20) is larger on an end portion side of the field magnet insertion hole in the circumferential direction than on the center side of the plurality of field magnet insertion holes (30) into which itself is inserted.
  • the at least one of the plurality of field magnets includes a plurality of field magnets, the plurality of field magnets inserted into the one of the plurality of field magnet insertion holes (30) being adjacent to each other in the circumferential direction (D) or in a direction parallel to the axis (P).
  • At least one of field magnets inserted into one field element insertion hole causes a field element core on a perimeter side of the field element insertion hole to function as one magnetic pole of the field element.
  • Magnetic poles that the field magnet insertion holes adjacent to each other in the circumferential direction cause the field element cores on the perimeter side thereof have polarities different from each other.
  • the first position is the center of the magnetic poles (magnetic pole center) and the second position is between the magnetic poles (between magnetic poles). The distance between the axis and the perimeter decreases from the first position toward the second position.
  • a magnetroresistance increases due to a decrease in the distance, with the result that the waveform of the magnetic flux density generated on the surface of the perimeter by the field magnet can be made close to a sinusoidal wave that is minimized between magnetic poles and maximized at the magnetic pole center.
  • the distance increases again between the magnetic poles.
  • the magnetic flux density is small between the magnetic poles, and thus the waveform of the magnetic flux density is only slightly affected even when the magnetroresistance is reduced. Therefore, in a case where an armature opposed to the field element is provided in the direction parallel to the rotation axis, it is possible to reduce a gap (air gap) between the field element and the armature between the magnetic poles while making the waveform of the magnetic flux density close to a sinusoidal wave.
  • the distance between the field element and the armature between the magnetic poles can be measured with ease. Accordingly, it is possible to increase the positions at which the distance between the field element and the armature is measured, and a relative position between the field element and the armature can be fixed with accuracy.
  • the magnetroresistance increases due to a decrease of the distance in the region in which the distance decreases from the first position toward the second position, and then the magnetroresistance can be increased due to the second cavity portion in the region in which the distance increases toward the second position.
  • an increase in magnetroresistance is decreased as closer to the first position.
  • the magnetroresistance can be adjusted base on a decrease in distance at the position close to the first position, whereby it is possible to finely adjust the magnetroresistance.
  • the first cavity portion and the second cavity portion are apart from each other, and thus the strength of the field element core can be enhanced.
  • the magnetroresistance increases due to a decrease of the distance in the region in which the distance decreases from the first position toward the second position, and then the magnetroresistance can be increased due to the cavity portion in the region in which the distance increases toward the second position.
  • an increase in magnetroresistance is reduced as closer to the first position.
  • the magnetroresistance can be adjusted based on a decrease of the distance at the position close to the first position, whereby it is possible to finely adjust the magnetroresistance.
  • the field magnets are tilted, toward the perimeter side, from the magnetic pole center to between the magnetic poles in one magnetic pole, and thus the magnetic flux density on the first position side can be enhanced. Accordingly, the magnetic flux density can be made closer to a sinusoidal wave.
  • the demagnetization resistance can be enhanced.
  • a high magnetic flux density can be generated at the center of the perimeter in the circumferential direction.
  • an eddy current flowing through the surface of the field magnet can be reduced. Normally, demagnetization is more likely to occur along with a temperature rise of the field magnet. Therefore, the Joule heat can be reduced by reducing the eddy current, and accordingly the demagnetization resistance can be enhanced.
  • FIG. 1 is a schematic cross-sectional view of a field element according to an embodiment of the present invention.
  • FIG. 1 shows the schematic structure of the field element in cross section perpendicular to a rotation axis P.
  • the field element includes a field element core 1 and a plurality of field magnets 20.
  • the field element core 1 has a perimeter 10 exposed around the rotation axis P, a plurality of field magnet insertion holes 30 circularly disposed around the rotation axis P, cavity portions 32, a shaft hole 40, and holes 50 for bolts or pins.
  • the shaft hole 40 is provided in a region including the rotation axis P while penetrating through the field element core 1 in a direction parallel to the rotation axis P. Note that the shaft hole 40 is not necessarily required. For example, the shaft hole 40 is not required in a mode in which end plates are provided to both ends of the field element core 1 in the direction parallel to the rotation axis P and a shaft is mounted to the end plates.
  • the holes 50 are disposed, for example, circularly around the rotation axis P and penetrate through the field element core 1 in the direction parallel to the rotation axis P.
  • a pin or bolt is inserted into the hole 50.
  • the field element core 1 is sandwiched between the end plates from both sides, and the entirety is fixed with pins or bolts through the holes 50.
  • the holes 50 are not necessarily required as long as there is provided a mode in which, for example, the field element core 1 and the end plates are fixed by welding.
  • the plurality of field magnet insertion holes 30 are circularly disposed around the rotation axis P. At least one field magnet is inserted into each of the field magnet insertion holes 30.
  • FIG. 1 illustrates a mode in which two field magnets 21 and 22 are inserted into each of the field magnet insertion holes 30.
  • the field magnets 21 and 22 cause the field element core 1 on the perimeter 10 side to function as magnetic poles. Note that in the description below, a pair of field magnets 21 and 22 inserted into one field magnet insertion hole 30 is referred to as the field magnet 20.
  • Magnetic pole surfaces of the field magnet 20 are disposed such that single magnetic pole faces the perimeter side.
  • the field magnets 21 and 22 respectively inserted into each of the field magnet insertion holes 30 are disposed with the magnetic pole surfaces of the same polarity facing the perimeter 10.
  • Polarities are different from each other between the magnetic pole surfaces on which the field magnets 21 and 22 that are inserted into one of a pair of adjacent field magnet insertion holes 30 in a circumferential direction D face the perimeter 10 and the magnetic pole surfaces on which the field magnets 21 and 22 that are inserted into the other thereof face the perimeter 10. Therefore, polarities are different from each other between the magnetic poles that the field magnet insertion holes 30 adjacent to each other in the circumferential direction D cause the field element core 1 on the perimeter 10 side thereof to function.
  • the field magnet insertion holes 30 may have cavity portions 31 at end portions in the circumferential direction thereof.
  • the cavity portions 31 are disposed on the side closer to the perimeter side than both ends of the field magnets 20.
  • the cavity portion 31 is not necessarily required, it is possible to reduce the leakage flux of the field magnet 20 by this.
  • the cavity portions 32 are disposed along the perimeter 10 on the center side (pole center 101 side described below) of the field magnet insertion hole 30 in the circumferential direction D with respect to the cavity portion 31 while being apart from the cavity portions 31 in the circumferential direction. Note that the cavity portion 32 is also necessarily required. The function of the cavity portion 32 is described below.
  • a radius R between the rotation axis P and the perimeter 10 is not uniform in accordance with the circumferential direction D.
  • the center of the field magnet insertion hole 30 in the circumferential direction D is referred to as a pole center 101.
  • the center of the field magnet insertion holes 30 adjacent to each other in the circumferential direction D is referred to as an interpole 102.
  • the radius R decreases from the pole center 101 toward the interpole 102 along the circumferential direction D in a monotonically non-increasing manner and then increases in a monotonically non-decreasing manner.
  • a rotating electric machine can be configured by disposing an armature so as to radially face the field element with the rotation axis P being the center.
  • the radius R decreases in a monotonically non-increasing manner from the pole center 101 toward the interpole 102. Therefore, a distance (air gap) between the field element and the armature increases from the pole center 101 toward the interpole 102. Accordingly, a magnetoresistance increases from the pole center 101 toward the interpole 102, and thus it is possible to make a waveform of the magnetic flux density generated by the field magnet 20 close to a sinusoidal wave.
  • the radius R increases again on the interpole 102 side.
  • the magnetic flux density generated by the field magnet 20 is small on the interpole 102 side, whereby the magnetroresistance only slightly affects the waveform of the magnetic flux density even when an air gap is reduced on the interpole 102 side and the magnetroresistance is reduced. Accordingly, the distance between the field element and the armature can be easily measured on the interpole 102 side even while making the waveform of the magnetic flux density close to a sinusoidal wave. As a result, it is possible to increase the positions at which the distance between the field element and the armature is measured, with the result that a relative position between the field element and the armature can be fixed with accuracy.
  • the cavity portion 32 has a shape in which a width in a radial direction with the rotation axis P being the center becomes narrower toward the pole center 101.
  • a point 11 on the perimeter 10 at which the radius R turns from decreasing to increasing in the circumferential direction D is positioned on the side closer to the interpole 102 than one end 321 of the cavity portion 32 on the pole center 101 in the circumferential direction D.
  • a rate of increase dR/d ⁇ of the radius R in the circumferential direction D is smaller than a rate of increase dH/d ⁇ of a width H of the cavity portion 32 in the radial direction at the same positions in the circumferential direction D.
  • a magnetroresistance is increased from the pole center 101 toward the interpole 102 by decreasing the radius R from the pole center 101 toward the interpole 102 in a monotonically non-increasing manner. Then, the magnetroresistance can be increased by the cavity portion 32 in the region in which the radius R increases. Accordingly, the magnetroresistance can be increased even in the region in which the radius R increases, and hence the magnetic flux density can be made close to a sinusoidal wave.
  • the magnetroresistance can be increased without reducing the radius R by the cavity portion 32, and thus the distance between the field element and the armature is not increased. Therefore, the distance can be measured easily even at a position at which the cavity portion 32 is positioned.
  • the cavity portion 32 in terms of fine adjustment of the magnetroresistance from the pole center 101 toward the interpole 102, decreasing the radius R depending on the circumferential direction is preferable to providing the cavity portion 32. This is because the shape of the cavity portion 32 on the one end 321 side is rounded in actuality, and thus fine adjustment of the width is limited in a region in which the width of the cavity portion 32 in the radial direction is small. Further, in a case where, for example, the cavity portion 32 is formed by punching, durability of a punching member becomes more problematic as the shape on the one end 321 side becomes sharper.
  • the radius R is reduced once from the pole center 101 side toward the interpole 102 to increase a magnetroresistance, and the magnetroresistance is increased by the cavity portion 32. Therefore, it is possible to prevent a reduction of the radius R on the interpole 102 side while finely adjusting the magnetroresistance on the pole center 101 side.
  • an angle of a tip shape of the cavity portion 32 on the one end side 321 is not required to be reduced, and thus the cavity portion 32 can be formed with ease. In a case where the cavity portion 32 is formed by punching, it is possible to improve the durability of the punching member.
  • the center of the field magnet insertion hole 30 in the circumferential direction D is positioned on the rotation axis P side with respect to a straight line connecting both ends of the field magnet 20 in the circumferential direction D. That is, the field magnets 21 and 22 are disposed in a V-shape. As a result, the magnetic flux density generated by the field magnets 21 and 22 can be concentrated on the pole center 101 side. Therefore, a waveform of the magnetic flux density can be made closer to a sinusoidal wave. Further, in this case, it is not required to reduce the magnetic flux density generated by the field magnet 20 by a magnetroresistance to be made close to a sinusoidal wave on the pole center 101 side.
  • the radius R can be made uniform from the pole center 101 to a predetermined region in the circumferential direction (region from the pole center 101 to a point 12 in FIG. 1 ; however, the point 12 is positioned on the pole center 101 side with respect to the point 11), and hence it is possible to effectively use the magnetic flux density generated by the field magnet 20.
  • FIG. 2 is a conceptual cross-sectional view showing another example of the field element according to the embodiment.
  • FIG. 2 shows a schematic structure of the field element in cross section perpendicular to the rotation axis P.
  • the field element core 1 has cavity portions 33 in place of the cavity portions 31 and 32.
  • the cavity portions 33 extend, from both ends of the field magnet 20 in the circumferential direction D, in a direction toward the perimeter 10 and in a direction toward the pole center 101 along the perimeter 10.
  • the cavity portion 32 has a shape in which a width thereof in the radial direction becomes narrower toward the pole center 101.
  • the point 11 at which the radius R turns from decreasing to increasing is positioned on the side closer to the interpole 102 than one end 331 of the cavity portion 33 in the circumferential direction D on the pole center 101 side. Further, a rate of increase of the radius R in the circumferential direction D is smaller than a rate of increase of the width of the cavity portion 33 in the radial direction at the same positions in the circumferential direction D.
  • the strength of the field element core 1 can be improved by providing the field element core 1 between the cavity portions 31 and 32 as shown in FIG. 1 .
  • the field element core 1 between the cavity portions 31 and 32 can be considered as a bridge.
  • FIG. 3 shows, in a motor including a conventional field element and an armature, magnetic flux lines and the magnetic flux density inside the field magnet when an opposing magnetic field is generated in the field magnet.
  • the conventional field element includes, for example, a field element core 7 and field magnets 70.
  • the field magnets 70 have a flat shape and are circularly disposed around the rotation axis P.
  • the armature is disposed so as to face the field element from the opposite side to the rotation axis P.
  • the armature includes an armature core 6 that includes teeth 61 protruding toward the rotation axis P side. Note that an armature winding wound around the teeth 61 is not shown.
  • FIG. 3 shows the magnetic flux lines and the magnetic flux density inside the field magnet 70 when one field magnet 70 faces one tooth 61. Further, the direction of the magnetic flux is indicated by a block arrow. The opposite magnetic field is applied to this one field magnet 70. The magnetic flux density on one end side of this one field magnet 70 in the circumferential direction D is shown under magnification. The magnitude of the magnetic flux density is indicated by contour lines 801 to 803. The contour lines 801 to 803 indicate that the magnetic flux density becomes smaller in this order.
  • a holding force of the field magnet 20 be larger on the end portion side of the field magnet insertion hole 30 than at the center of the field magnet insertion hole 30 in the circumferential direction D.
  • the demagnetization resistance can be enhanced on the end portion side of the field magnet 20.
  • an energy product of the field magnet 20 be larger on the end portion side of the field magnet insertion hole 30 than on the center side of the field magnet insertion hole 30. Accordingly, it is possible to generate a high magnetic flux density at the center of the perimeter 10 in the circumferential direction D.
  • FIGS. 1 and 2 two field magnets 21 and 22 are inserted into one field magnet insertion hole 30, and the field magnets 21 and 22 are adjacent to each other in the direction parallel to the circumferential direction D.
  • An insulator exists between the field magnets 21 and 22, with the result that an eddy current flowing through the field magnet 20 can be reduced.
  • the field magnet tends to be subjected to demagnetization along with a temperature rise thereof. Therefore, the Joule heat can be reduced by reducing an eddy current, and thus the demagnetization resistance can be enhanced.
  • the field magnets 21 and 22 may be adjacent to each other in the direction parallel to the rotation axis P. Alternatively, three or more field magnets may be inserted into one field magnet through hole 30.

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)
  • Iron Core Of Rotating Electric Machines (AREA)

Claims (6)

  1. Élément de champ, comprenant:
    une pluralité d'inducteurs (20, 21, 22) ; et
    un noyau d'élément de champ (1) présentant :
    un périmètre (10) exposé autour d'un axe (P) prédéterminé ; et
    une pluralité de trous d'insertion d'inducteur (30, 31, 33) disposés de manière circulaire autour dudit axe, dans lesquels au moins l'un de ladite pluralité d'inducteurs est inséré dans chacun desdits au moins un de ladite pluralité de trous d'insertion d'inducteur, dans lequel :
    ledit au moins un de ladite pluralité d'inducteurs insérés dans chacun de ladite pluralité de trous d'insertion d'inducteur est disposé avec une surface de pôle magnétique d'une polarité unique faisant face audit périmètre ;
    l'un de ladite pluralité de trous d'insertion d'inducteur et un autre de ladite pluralité de trous d'insertion d'inducteur sont adjacents l'un à l'autre dans une direction circonférentielle (D) avec ledit axe en tant que centre, où ladite surface de pôle magnétique dudit au moins un de ladite pluralité d'inducteurs insérés dans ledit un de ladite pluralité de trous d'insertion d'inducteur et ladite surface de pôle magnétique dudit au moins un de ladite pluralité d'inducteurs insérés dans ledit un autre de ladite pluralité de trous d'insertion d'inducteur sont différentes l'une de l'autre en polarité ; et
    entre une première position (101) dans ladite direction circonférentielle au niveau de laquelle un centre dudit un de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle est positionné et une seconde position (102) dans ladite direction circonférentielle au niveau de laquelle un centre entre ledit un de ladite pluralité de trous d'insertion d'inducteur et ledit un autre de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle est positionné, une distance (R) entre ledit axe et ledit périmètre diminue d'une manière décroissante monotone depuis ladite première position vers ladite seconde position le long de ladite direction circonférentielle et elle augmente ensuite d'une manière croissante monotone ;
    l'élément de champ étant caractérisé en ce que :
    chacun de ladite pluralité de trous d'insertion d'inducteur présente, au niveau des deux extrémités dans ladite direction circonférentielle (D), des premières parties formant cavité (31) sur un côté plus près dudit périmètre (10) que ledit au moins un de ladite pluralité d'inducteurs (21, 22) insérés dans celles-ci ;
    ledit noyau d'élément de champ (1) présente en outre des secondes parties formant cavité (32) disposées chacune le long dudit périmètre sur ledit côté de première position (101) par rapport auxdites premières parties formant cavité, à l'écart desdites premières parties formant cavité dans ladite direction circonférentielle (D) ; et
    un point (11) sur ledit périmètre au niveau duquel ladite distance (R) passe d'une diminution à une augmentation entre ladite première position et ladite seconde position est positionné sur un côté plus près de ladite seconde position dans ladite direction circonférentielle qu'une extrémité (321) de ladite seconde partie formant cavité sur ledit côté de première position dans ladite direction circonférentielle.
  2. Élément de champ, comprenant:
    une pluralité d'inducteurs (20, 21, 22) ; et
    un noyau d'élément de champ (1) présentant :
    un périmètre (10) exposé autour d'un axe (P) prédéterminé ; et
    une pluralité de trous d'insertion d'inducteur (30, 31, 33) disposés de manière circulaire autour dudit axe, dans lesquels au moins un de ladite pluralité d'inducteurs est inséré dans chacun desdits au moins un de ladite pluralité de trous d'insertion d'inducteur, dans lequel :
    ledit au moins un de ladite pluralité d'inducteurs insérés dans chacun de ladite pluralité de trous d'insertion d'inducteur est disposé avec une surface de pôle magnétique d'une polarité unique faisant face audit périmètre ;
    un de ladite pluralité de trous d'insertion d'inducteur et un autre de ladite pluralité de trous d'insertion d'inducteur sont adjacents l'un à l'autre dans une direction circonférentielle (D) avec ledit axe en tant que centre, où ladite surface de pôle magnétique dudit au moins un de ladite pluralités d'inducteurs insérés dans ledit un de ladite pluralité de trous d'insertion d'inducteur et ladite surface de pôle magnétique dudit au moins un de ladite pluralité d'inducteurs insérés dans ledit un autre de ladite pluralité de trous d'insertion d'inducteur sont différents l'un de l'autre en polarité ; et
    entre une première position (101) dans ladite direction circonférentielle au niveau de laquelle un centre dudit un de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle est positionné et une seconde position (102) dans ladite direction circonférentielle au niveau de laquelle un centre entre ledit un de ladite pluralité de trous d'insertion d'inducteur et ledit un autre de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle est positionné, une distance (R) entre ledit axe et ledit périmètre diminue d'une manière décroissante monotone depuis ladite première position vers ladite seconde position le long de ladite direction circonférentielle et elle augmente ensuite d'une manière croissante monotone ;
    l'élément de champ étant caractérisé en ce que :
    chacun de ladite pluralité de trous d'insertion d'inducteur (30) présente, au niveau des deux extrémités dans ladite direction circonférentielle (D), des parties formant cavité (33) sur un côté plus près dudit périmètre (10) que ledit au moins un de ladite pluralité d'inducteurs (21, 22) insérés dans celles-ci, les parties formant cavité (33) s'étendant dans une direction vers ledit périmètre (10) et une direction vers ladite première position (101) le long dudit périmètre ; et
    un point (11) sur ledit périmètre (10) au niveau duquel ladite distance (R) passe d'une diminution à une augmentation entre ladite première position (101) et ladite seconde position (102) est positionné sur un côté plus près de ladite seconde position dans ladite direction circonférentielle qu'une extrémité (321) de ladite seconde partie formant cavité sur ledit côté de première position dans ladite direction circonférentielle.
  3. Élément de champ selon la revendication 1 ou 2, dans lequel ledit centre dudit un de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle (D) est positionné sur le côté dudit axe (P) par rapport à une ligne droite reliant les deux extrémités dans ladite direction circonférentielle dudit au moins un de ladite pluralité d'inducteurs insérés dans ledit un de ladite pluralité de trous d'insertion d'inducteur (30).
  4. Élément de champ selon l'une quelconque des revendications 1 à 3, dans lequel une force coercitive dudit au moins un de ladite pluralité d'inducteurs (20) est plus grande sur un côté partie d'extrémité d'un de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle que sur ledit côté centre dudit un de ladite pluralité de trous d'insertion d'inducteur (30) dans lequel il est lui-même inséré.
  5. Élément de champ selon l'une quelconque des revendications 1 à 4, dans lequel un produit énergétique dudit au moins un de ladite pluralité d'inducteurs (20) est plus grand sur un côté partie d'extrémité d'un de ladite pluralité de trous d'insertion d'inducteur dans ladite direction circonférentielle que sur ledit côté centre dudit un de ladite pluralité de trous d'insertion d'inducteur (30) dans lesquels il est lui-même inséré.
  6. Élément de champ selon l'une quelconque des revendications 1 à 5, dans lequel ledit au moins un de ladite pluralité d'inducteurs comprend une pluralité d'inducteurs, ladite pluralité d'inducteurs insérés dans ledit un de ladite pluralité de trous d'insertion d'inducteur (30) étant adjacents les uns aux autres dans ladite direction circonférentielle (D) ou dans une direction parallèle audit axe (P).
EP09742670.4A 2008-05-08 2009-04-22 Elément de champ Not-in-force EP2280470B1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP2008122256A JP5380900B2 (ja) 2008-05-08 2008-05-08 界磁子
PCT/JP2009/057994 WO2009136545A1 (fr) 2008-05-08 2009-04-22 Elément de champ

Publications (3)

Publication Number Publication Date
EP2280470A1 EP2280470A1 (fr) 2011-02-02
EP2280470A4 EP2280470A4 (fr) 2017-04-12
EP2280470B1 true EP2280470B1 (fr) 2020-10-07

Family

ID=41264600

Family Applications (1)

Application Number Title Priority Date Filing Date
EP09742670.4A Not-in-force EP2280470B1 (fr) 2008-05-08 2009-04-22 Elément de champ

Country Status (7)

Country Link
US (1) US8598763B2 (fr)
EP (1) EP2280470B1 (fr)
JP (1) JP5380900B2 (fr)
KR (1) KR101173387B1 (fr)
CN (1) CN102017367B (fr)
AU (1) AU2009245221B2 (fr)
WO (1) WO2009136545A1 (fr)

Families Citing this family (43)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5565170B2 (ja) * 2010-07-27 2014-08-06 富士電機株式会社 永久磁石式回転機
JP5685952B2 (ja) * 2011-01-21 2015-03-18 ダイキン工業株式会社 回転子
JP5652221B2 (ja) * 2011-01-21 2015-01-14 ダイキン工業株式会社 回転子
JP5811565B2 (ja) * 2011-03-31 2015-11-11 株式会社富士通ゼネラル 回転子および永久磁石電動機
JP5811567B2 (ja) * 2011-03-31 2015-11-11 株式会社富士通ゼネラル 回転子および永久磁石電動機
EP2592718A2 (fr) * 2011-11-08 2013-05-15 Kabushiki Kaisha Yaskawa Denki Noyau de rotor, rotor et machine tournante électrique
JP2013126272A (ja) * 2011-12-13 2013-06-24 Samsung Electronics Co Ltd モータ
JP2013126281A (ja) * 2011-12-14 2013-06-24 Daikin Ind Ltd 界磁子の製造方法及び界磁子用の端板
US10153671B2 (en) * 2011-12-29 2018-12-11 Philip Totaro Permanent magnet rotor with intrusion
WO2013141323A1 (fr) 2012-03-23 2013-09-26 三菱重工オートモーティブサーマルシステムズ株式会社 Moteur et compresseur électrique utilisant ce moteur
JP5901436B2 (ja) * 2012-06-08 2016-04-13 日立アプライアンス株式会社 永久磁石同期機
WO2013187439A1 (fr) * 2012-06-14 2013-12-19 ダイキン工業株式会社 Machine électrique tournante de type à aimant intégré
JP5920472B2 (ja) * 2012-08-29 2016-05-18 株式会社安川電機 回転電機およびロータ
DE102013201199A1 (de) * 2013-01-25 2014-07-31 Magna Powertrain Ag & Co. Kg Elektrische Maschine und Verfahren zur Herstellung eines Elektroblechs
JP6110151B2 (ja) * 2013-02-07 2017-04-05 本田技研工業株式会社 回転電機のロータ
CN103337921A (zh) * 2013-06-27 2013-10-02 信质电机股份有限公司 用于变频调速电动机的转子结构以及一种具有该转子结构的变频调速电动机
CN104300710B (zh) * 2013-07-17 2018-09-04 丹佛斯（天津）有限公司 转子、内置式永磁电机以及压缩机
JP2015122936A (ja) * 2013-10-31 2015-07-02 三星電子株式会社Ｓａｍｓｕｎｇ Ｅｌｅｃｔｒｏｎｉｃｓ Ｃｏ．，Ｌｔｄ． 埋込磁石型モータ及び埋込磁石型モータの使用方法
US10205359B2 (en) 2013-11-18 2019-02-12 Steering Solutions Ip Holding Corporation Low cost permanent magnet motor for an electric power steering system
JP6157340B2 (ja) * 2013-12-18 2017-07-05 三菱電機株式会社 永久磁石式回転電機
CN106233580B (zh) * 2014-04-28 2019-07-09 三菱电机株式会社 转子、永久磁铁埋入式电动机以及压缩机
JP6327348B2 (ja) * 2014-08-11 2018-05-23 富士電機株式会社 回転電機
CN106030989B (zh) * 2014-08-11 2018-09-11 富士电机株式会社 旋转电机
JP6210160B2 (ja) * 2014-08-11 2017-10-11 富士電機株式会社 同期リラクタンス回転電機
US9979243B2 (en) * 2014-11-18 2018-05-22 Steering Solutions Ip Holding Corporation Low cost injection molded buried permanent magnet motor for an electric power steering system
KR20160114879A (ko) * 2015-03-25 2016-10-06 삼성전자주식회사 로터, 이를 포함하는 모터, 및 그 제조방법
JP6506649B6 (ja) * 2015-07-27 2019-06-05 日立グローバルライフソリューションズ株式会社 永久磁石同期機及びそれを用いた機器
JP6507273B2 (ja) * 2015-12-18 2019-04-24 ハノン システムズ 永久磁石埋込型電動機のためのロータ及びそれを用いた電動機
KR102526938B1 (ko) * 2015-12-18 2023-05-02 한온시스템 주식회사 영구자석 매립형 전동기를 위한 로터 및 그를 이용한 전동기
CN105932804A (zh) * 2016-06-20 2016-09-07 广东威灵电机制造有限公司 用于电机的转子和具有其的电机
JP6826412B2 (ja) * 2016-10-07 2021-02-03 東芝産業機器システム株式会社 同期リラクタンス型回転電機
DE102017201029A1 (de) * 2017-01-23 2018-07-26 Audi Ag Rotor für elektrische Maschine
CN109149811A (zh) * 2017-06-27 2019-01-04 上海电驱动股份有限公司 一种永磁同步电机的转子冲片
TWM576750U (zh) 2017-07-25 2019-04-11 美商米沃奇電子工具公司 電氣組合物、電動化裝置系統、電池組、電馬達、馬達總成及電馬達總成
CN107516954A (zh) * 2017-10-24 2017-12-26 东莞市博瓦特动力科技有限公司 一种抗去磁的纯正弦波永磁电机转子
US20190252934A1 (en) * 2018-02-13 2019-08-15 New Widetech Industries Co., Ltd. Motor rotor with holes
CN108988527A (zh) * 2018-06-27 2018-12-11 德威(苏州)新能源有限公司 一种混合励磁高功率密度磁阻永磁电机转子
EP3917708A4 (fr) 2019-02-18 2022-11-30 Milwaukee Electric Tool Corporation Outil à percussion
US20220399764A1 (en) * 2019-11-12 2022-12-15 Mavel edt S.p.A. Synchronous electric machine with reluctance assisted by permanent magnets and process for making such electric machine
GB2597239B (en) * 2020-06-26 2023-04-26 Jaguar Land Rover Ltd Rotor assembly
FR3115949B1 (fr) * 2020-11-05 2025-06-20 Valeo Equip Electr Moteur Rotor de machine électrique tournante
JP7600730B2 (ja) * 2021-02-09 2024-12-17 スズキ株式会社 回転電機
JP7134278B1 (ja) * 2021-02-25 2022-09-09 三菱電機株式会社 回転電機

Family Cites Families (22)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08340651A (ja) * 1995-06-12 1996-12-24 Toshiba Corp 永久磁石及び永久磁石形回転電機
JPH0993996A (ja) * 1995-09-28 1997-04-04 Yoshiaki Takahashi 発電電動機
EP0823771B1 (fr) * 1996-02-23 2006-04-26 Matsushita Electric Industrial Co., Ltd. Moteur
TW364234B (en) * 1997-04-14 1999-07-11 Sanyo Electric Co Rotor for an electric motor
JP3280896B2 (ja) * 1997-10-31 2002-05-13 株式会社東芝 永久磁石式リラクタンス型回転電機
US6087751A (en) 1997-07-01 2000-07-11 Kabushiki Kaisha Toshiba Reluctance type rotating machine with permanent magnets
JP3818339B2 (ja) * 1997-09-22 2006-09-06 株式会社富士通ゼネラル 永久磁石電動機
JP4084889B2 (ja) * 1998-07-23 2008-04-30 アイチエレック株式会社 永久磁石形電動機の回転子
JP2000217287A (ja) * 1999-01-19 2000-08-04 Toshiba Corp 永久磁石形モ―タ及びコンプレッサ
US6563246B1 (en) * 1999-10-14 2003-05-13 Denso Corporation Rotary electric machine for electric vehicle
JP3602392B2 (ja) * 1999-12-21 2004-12-15 アイチエレック株式会社 永久磁石埋め込みモータ
TW577658U (en) 2001-09-10 2004-02-21 Adlee Powertronic Co Ltd Rotor structure for a motor having built-in type permanebt magnet
JP3684344B2 (ja) 2001-11-02 2005-08-17 三菱電機株式会社 永久磁石回転子およびその製造方法
JP2004104962A (ja) 2002-09-12 2004-04-02 Toshiba Industrial Products Manufacturing Corp 永久磁石式リラクタンス型回転電機
TW200509515A (en) * 2003-07-04 2005-03-01 Daikin Ind Ltd Motor
JP4449035B2 (ja) * 2004-03-10 2010-04-14 日立オートモティブシステムズ株式会社 電動車両用の永久磁石回転電機
JP4815204B2 (ja) * 2005-12-01 2011-11-16 アイチエレック株式会社 永久磁石回転機及び圧縮機
JP4131276B2 (ja) 2005-12-19 2008-08-13 ダイキン工業株式会社 電動機並びにその回転子及び回転子用磁心
JP4135018B2 (ja) * 2006-04-24 2008-08-20 株式会社富士通ゼネラル 磁石埋め込み型回転子、この回転子を用いた電動機及びこの電動機を用いた圧縮機
US7851958B2 (en) * 2006-06-12 2010-12-14 Remy International, Inc. Electric machine with interior permanent magnets
JP2007300796A (ja) 2007-07-17 2007-11-15 Aichi Elec Co 永久磁石形電動機の回転子
US7808143B2 (en) * 2007-10-24 2010-10-05 Rechi Precision Co., Ltd. Permanent magnet motor

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
None *

Also Published As

Publication number Publication date
WO2009136545A1 (fr) 2009-11-12
KR101173387B1 (ko) 2012-08-10
CN102017367A (zh) 2011-04-13
CN102017367B (zh) 2014-12-24
US20110062815A1 (en) 2011-03-17
AU2009245221A1 (en) 2009-11-12
EP2280470A1 (fr) 2011-02-02
KR20100134731A (ko) 2010-12-23
EP2280470A4 (fr) 2017-04-12
JP2009273258A (ja) 2009-11-19
US8598763B2 (en) 2013-12-03
AU2009245221B2 (en) 2013-08-22
JP5380900B2 (ja) 2014-01-08

Similar Documents

Publication Publication Date Title
EP2280470B1 (fr) Elément de champ
EP1286446B1 (fr) Rotor et machine à aimants permanents
JP5288698B2 (ja) 永久磁石式リラクタンス型回転電機
US8937418B2 (en) Rotor core, rotor, and rotating electric machine
US9716411B2 (en) Permanent-magnet-type rotating electric mechanism
JP5533879B2 (ja) 永久磁石形回転電機の回転子
US12191713B2 (en) Rotor of rotary electric machine
JP2014039475A (ja) Ｐｍシンクロナスモータ
CN102457114A (zh) 旋转电机
JP2014093858A (ja) 回転電機のロータ
JP2005204477A (ja) 回転電機の着磁装置、及び回転電機の着磁方法
JP5589662B2 (ja) 分割型回転子及び電動機
KR20150114879A (ko) 로터 및 이를 이용하는 모터
CN212486223U (zh) 转子及马达
JP2013179837A (ja) 界磁子
US12512711B2 (en) Rotor with magnet and embedding holes
JP4714512B2 (ja) モータの回転子及び回転子の製造方法
CA2604812C (fr) Rotor a haute vitesse

Legal Events

Date Code Title Description
PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

17P Request for examination filed

Effective date: 20101105

AK Designated contracting states

Kind code of ref document: A1

Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO SE SI SK TR

AX Request for extension of the european patent

Extension state: AL BA RS

DAX Request for extension of the european patent (deleted)
RA4 Supplementary search report drawn up and despatched (corrected)

Effective date: 20170313

RIC1 Information provided on ipc code assigned before grant

Ipc: H02K 1/22 20060101ALI20170307BHEP

Ipc: H02K 1/27 20060101AFI20170307BHEP

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: EXAMINATION IS IN PROGRESS

17Q First examination report despatched

Effective date: 20180716

GRAP Despatch of communication of intention to grant a patent

Free format text: ORIGINAL CODE: EPIDOSNIGR1

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: GRANT OF PATENT IS INTENDED

INTG Intention to grant announced

Effective date: 20200507

GRAS Grant fee paid

Free format text: ORIGINAL CODE: EPIDOSNIGR3

GRAA (expected) grant

Free format text: ORIGINAL CODE: 0009210

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE PATENT HAS BEEN GRANTED

AK Designated contracting states

Kind code of ref document: B1

Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO SE SI SK TR

REG Reference to a national code

Ref country code: GB

Ref legal event code: FG4D

REG Reference to a national code

Ref country code: CH

Ref legal event code: EP

Ref country code: AT

Ref legal event code: REF

Ref document number: 1322205

Country of ref document: AT

Kind code of ref document: T

Effective date: 20201015

REG Reference to a national code

Ref country code: DE

Ref legal event code: R096

Ref document number: 602009062885

Country of ref document: DE

REG Reference to a national code

Ref country code: IE

Ref legal event code: FG4D

REG Reference to a national code

Ref country code: NL

Ref legal event code: MP

Effective date: 20201007

REG Reference to a national code

Ref country code: AT

Ref legal event code: MK05

Ref document number: 1322205

Country of ref document: AT

Kind code of ref document: T

Effective date: 20201007

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: PT

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20210208

Ref country code: NO

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20210107

Ref country code: NL

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: FI

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: GR

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20210108

REG Reference to a national code

Ref country code: LT

Ref legal event code: MG4D

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: BG

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20210107

Ref country code: AT

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: IS

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20210207

Ref country code: ES

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: SE

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: LV

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: PL

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: HR

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

REG Reference to a national code

Ref country code: DE

Ref legal event code: R097

Ref document number: 602009062885

Country of ref document: DE

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: LT

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: RO

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: SK

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: EE

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: CZ

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

PLBE No opposition filed within time limit

Free format text: ORIGINAL CODE: 0009261

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: NO OPPOSITION FILED WITHIN TIME LIMIT

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: DK

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

26N No opposition filed

Effective date: 20210708

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: IT

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: SI

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

Ref country code: MC

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: LU

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20210422

REG Reference to a national code

Ref country code: BE

Ref legal event code: MM

Effective date: 20210430

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: CH

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20210430

Ref country code: LI

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20210430

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: IE

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20210422

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: IS

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20210207

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: BE

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20210430

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: HU

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT; INVALID AB INITIO

Effective date: 20090422

Ref country code: CY

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

P01 Opt-out of the competence of the unified patent court (upc) registered

Effective date: 20230525

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: MK

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

PGFP Annual fee paid to national office [announced via postgrant information from national office to epo]

Ref country code: GB

Payment date: 20240229

Year of fee payment: 16

PGFP Annual fee paid to national office [announced via postgrant information from national office to epo]

Ref country code: FR

Payment date: 20240308

Year of fee payment: 16

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: TR

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

PGFP Annual fee paid to national office [announced via postgrant information from national office to epo]

Ref country code: DE

Payment date: 20240227

Year of fee payment: 16

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: MT

Free format text: LAPSE BECAUSE OF FAILURE TO SUBMIT A TRANSLATION OF THE DESCRIPTION OR TO PAY THE FEE WITHIN THE PRESCRIBED TIME-LIMIT

Effective date: 20201007

REG Reference to a national code

Ref country code: DE

Ref legal event code: R119

Ref document number: 602009062885

Country of ref document: DE

GBPC Gb: european patent ceased through non-payment of renewal fee

Effective date: 20250422

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: DE

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20251104

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: GB

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20250422

PG25 Lapsed in a contracting state [announced via postgrant information from national office to epo]

Ref country code: FR

Free format text: LAPSE BECAUSE OF NON-PAYMENT OF DUE FEES

Effective date: 20250430